CN108346739A - A kind of Ge-Sb-C phase-change storage materials, preparation method and application - Google Patents

A kind of Ge-Sb-C phase-change storage materials, preparation method and application Download PDF

Info

Publication number
CN108346739A
CN108346739A CN201810097825.8A CN201810097825A CN108346739A CN 108346739 A CN108346739 A CN 108346739A CN 201810097825 A CN201810097825 A CN 201810097825A CN 108346739 A CN108346739 A CN 108346739A
Authority
CN
China
Prior art keywords
phase
change storage
change
storage materials
materials
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN201810097825.8A
Other languages
Chinese (zh)
Other versions
CN108346739B (en
Inventor
徐�明
吴倩倩
缪向水
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Huazhong University of Science and Technology
Original Assignee
Huazhong University of Science and Technology
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Huazhong University of Science and Technology filed Critical Huazhong University of Science and Technology
Priority to CN201810097825.8A priority Critical patent/CN108346739B/en
Publication of CN108346739A publication Critical patent/CN108346739A/en
Application granted granted Critical
Publication of CN108346739B publication Critical patent/CN108346739B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N70/00Solid-state devices without a potential-jump barrier or surface barrier, and specially adapted for rectifying, amplifying, oscillating or switching
    • H10N70/801Constructional details of multistable switching devices
    • H10N70/881Switching materials
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N70/00Solid-state devices without a potential-jump barrier or surface barrier, and specially adapted for rectifying, amplifying, oscillating or switching
    • H10N70/011Manufacture or treatment of multistable switching devices
    • H10N70/021Formation of the switching material, e.g. layer deposition
    • H10N70/026Formation of the switching material, e.g. layer deposition by physical vapor deposition, e.g. sputtering
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10NELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10N70/00Solid-state devices without a potential-jump barrier or surface barrier, and specially adapted for rectifying, amplifying, oscillating or switching
    • H10N70/011Manufacture or treatment of multistable switching devices
    • H10N70/041Modification of the switching material, e.g. post-treatment, doping
    • H10N70/043Modification of the switching material, e.g. post-treatment, doping by implantation

Abstract

The invention belongs to microelectronics technologies, and in particular to a kind of Ge Sb C phase-change storage materials, preparation method and application.The Ge Sb C New-type phase change storage materials of the present invention, chemical composition general formula (GeiSbj)100‑xCx, wherein x, i, j indicate atomic percent, 0 < x <, 15,0 < i≤50,50≤j < 100, i+j=100.Compared with prior art, a kind of Ge Sb C phase-change storage materials of the invention before phase change after variable density reduce so that the stress that is generated after phase transformation reduces, and device cycle performance improves;In the present invention simultaneously, the Ge Sb C phase-change storage material phase transition temperatures are improved significantly, thermal stability enhancing, data retention enhancing;In addition, the crystalline resistance rate of the Ge Sb C phase-change storage materials increases, the RESET electric currents of device reduce, and operate lower power consumption.

Description

A kind of Ge-Sb-C phase-change storage materials, preparation method and application
Technical field
The invention belongs to microelectronics technologies, and in particular to a kind of Ge-Sb-C phase-change storage materials, preparation method and Using.
Background technology
Phase transition storage (PCRAM) be based on phase-change storage material (mainly chalcogenide compound) crystal and it is noncrystal it Between rapid translating realize the storage of " 0 " and " 1 ".In phase-change memory cell, it is only necessary to utilize narrow spaces, an amplitude Electric pulse operate on it (RESET operation), crystalline phase-change storage material will melt rapid cooling, be changed into amorphous state, from And it realizes from low resistance state " 0 " to the quick resistive of high-resistance state " 1 ".Conversely, applying wide pulse width, low amplitude value to device Electric pulse (SET operation), amorphous state phase-change storage material will crystallize phase transformation, return to low resistance state.Phase transition storage has read-write The advantages that speed is fast, storage density is high, mutually compatible with traditional cmos process.
(Ge2Sb2Te5) GST is widely studied as traditional phase-change storage material and in the industrialization of phase transition storage It is middle to be applied, but research shows that the presence of sulphur series elements Te will produce some seondary effects, influence the performance (Krusin- of device Elbaum,L.,et al.,Evidence for segregation of Te in Ge2Sb2Te5films:Effect on the“phase-change”stress.Applied Physics Letters,2007.90(14):p.141902).First, Te The diffusion coefficient of element is higher, is spread easily in phase-change memory cell and interacts with neighbouring Te elements and lead to Te simple substance Phase separation;Meanwhile Te elements easily assemble generation stress in grain boundaries, to influence the cycling durable performance of device;It is most important It is that, due to the intrinsic vacancy there are 10% or so in crystalline state GST, during mutually becoming amorphous, these vacancy can assemble At 16%~17% or so amorphous cavity, so that the volume differences (density contrast) after before phase change reach 6%~7%, shadow Ring its service life (Njoroge, W.K., H.-W. as deviceand M.Wuttig,Density changes upon crystallization of Ge2Sb2.04Te4.74films.Journal of Vacuum Science& Technology A:Vacuum,Surfaces,and Films,2002.20(1):p.230-233).High density storage in this A problem is with regard to even more serious, because in three-dimensional high-density storage, the stress that device density variation generates will be applied, to Cause the failure of storage array.
And in Ge-Sb materials, the missing of Te elements is expected to solve the above problems.It is accounted in addition, Ge-Sb belongs to grain growth Leading type material, crystallization rate is quickly;And component ratio is Ge15Sb85Phase transition temperature be 250 DEG C of (Zalden, P., et al.,Atomic structure of amorphous and crystallized Ge15Sb85.Journal of Applied Physics,2010.107(10):P.104312), high than phase transition temperature (156 DEG C) of traditional phase-change storage material GST, energy Its amorphous state thermal stability is effectively improved to improve the data storage capacities of device, while reducing the heat string between storage unit It disturbs;And in crystalline state Ge-Sb be not present intrinsic vacancy, therefore before phase change after variable density ratio GST it is small.But Ge-Sb is in phase The PHASE SEPARATION that will appear rich Ge and richness Sb during becoming, influences the recycling performance of device.In order to further decrease Ge-Sb Variable density after before phase change promotes the performance of Ge-Sb, it is therefore desirable to modification is doped to this.
Invention content
For the disadvantages described above or Improvement requirement of the prior art, the present invention provides a kind of Ge-Sb-C phase-change storage materials, Preparation method and application, its object is to by the way that carbon is introduced in the Ge-Sb phase-change storage materials of the prior art, phase It obtains a kind of Ge-Sb-C phase-change storage materials for phase transition storage with answering, phase-change storage material can be reduced in phase Become front and back variable density, improve phase-change storage material thermal stability, improve the cycling durable performance of memory device, reduces memory Operation power consumption of part etc..
To achieve the above object, according to one aspect of the present invention, a kind of Ge-Sb-C phase-change storage materials are provided, Chemical composition general formula is (GeiSbj)100-xCx, wherein x, i, j are atomic percent, wherein 0 < x < 15,0 < i≤50,50 ≤ j < 100, i+j=100.
Preferably, the phase-change storage material, 0 < x <, 6,0 < i≤20,80≤j < 100, i+j=100.
Preferably, C atoms are present in Ge-Sb interstitial voids in the Ge-Sb-C phase-change storage materials, and and Ge-Sb Form chemical bond.
Preferably, the Ge-Sb-C phase-change storage materials are Ge-Sb-C phase change film materials.
Preferably, the thickness of the film is 20-200nm.
Preferably, the Ge-Sb-C phase-change storage materials control the phase change memory material by controlling the incorporation content of C The phase transition temperature and resistivity of material.
Preferably, the resistivity of the high-impedance state of the Ge-Sb-C phase-change storage materials is at least 100 times of low resistance state.
Other side according to the invention provides a kind of preparation method of the phase-change storage material, is magnetic Control sputtering method, chemical vapour deposition technique, atomic layer deposition method, galvanoplastic or electron-beam vapor deposition method.
Preferably, the preparation method is magnetron sputtering method, and specific magnetron sputtering mode is in following four mode Any one:(1) C, Ge and Sb target co-sputtering;(2) C and GeiSbjCosputtering;(3) Ge after C dopingiSbjAlloys target sputters (4) graphite flake is directly placed at GeiSbjSputtering is doped on alloy target material.
Other side according to the invention provides a kind of Ge-Sb-C phase-change storage materials in phase transition storage In application.
In general, through the invention it is contemplated above technical scheme is compared with the prior art, can obtain down and show Beneficial effect:
Compared with Ge-Sb phase-change storage materials undoped in the prior art, Ge-Sb-C phase-change materials of the invention In, C is atom doped in Ge-Sb interstitial voids, and forms tetrahedron center in amorphous state and improve atom packing efficiency, Ge- Sb-C phase-change storage materials before phase change after variable density reduce so that the stress that is generated after phase transformation reduces, and device cycle is durable Performance improves;In the present invention simultaneously, the phase transition temperature of the Ge-Sb-C phase-change storage materials is improved significantly, and heat is steady Qualitative enhancing enhances to the data retention of device;In addition, the crystalline resistance rate liter of the Ge-Sb-C phase-change storage materials The RESET electric currents of height, device reduce, and operate lower power consumption.
Description of the drawings
Fig. 1 is the Ge-Sb-C phase-change storage materials of difference C doping contents of the invention and the Ge-Sb phase transformations for comparative example 1 The front and back X ray reflection rate pattern of storage material annealing.Crystalline state sample is annealed 10min at 250 DEG C.
Fig. 2 is the Ge-Sb-C phase-change storage materials with the AFM difference C doping contents of the invention measured and is used for comparative example 1 The annealing that is characterized with thickness of Ge-Sb phase-change storage materials before and after volume (density) variation with C doping contents change curve. Crystalline state sample is annealed 10min at 250 DEG C.
Fig. 3 is the Ge-Sb-C phase-change storage materials of different C contents of the invention and the Ge-Sb phase change memories for comparative example 1 The In-situ resistance rate of material and the relation curve of annealing temperature, wherein heating rate are 5 DEG C/min.
Fig. 4 be in the present invention with first-principles calculations when C doping contents be 5% amorphous state Ge-Sb-C bond distance, Bond angle and ligancy situation.
Fig. 5 is the amorphous state Ge-Sb-C phase transformation materials for being 5% when C doping contents with first-principles calculations in the present invention Super born of the same parents' model of material.
Fig. 6 is in the present invention with C in the Ge-Sb-C phase-change storage materials of the different C doping contents of first-principles calculations The formational situation of chain.
Specific implementation mode
In order to make the purpose , technical scheme and advantage of the present invention be clearer, with reference to the accompanying drawings and embodiments, right The present invention is further elaborated.It should be appreciated that the specific embodiments described herein are merely illustrative of the present invention, and It is not used in the restriction present invention.As long as in addition, technical characteristic involved in the various embodiments of the present invention described below It does not constitute a conflict with each other and can be combined with each other.
The present invention provides a kind of Ge-Sb-C phase-change storage materials, for C is introduced to Ge-Sb phase-change storage material bodies It is obtained in system, chemical composition general formula is (GeiSbj)100-xCx, in GeiSbjC is adulterated on the basis of material, obtains Ge-Sb-C Phase-change storage material.X, i, j are atomic percent, wherein 0 < x <, 15,0 < i≤50,50≤j < 100, i+j=100.Compared with Good, the value range of the x is 0 < x < 6, and the value range of further preferably 2 < x < 6, i are taking for 0 < i≤20, j It is worth ranging from 80≤x < 100, and i+j=100.In the Ge-Sb-C phase-change storage materials, the C atoms of incorporation are in Ge-Sb crystalline substances The interstitial site of lattice, and with Ge, Sb at chemical bond.As a preferred option, the Ge-Sb-C phase-change storage materials are Ge- Sb-C phase change film materials.Preferably, the thickness of Ge-Sb-C phase change film materials is 20nm-200nm.
The institute that the front and back change in film thickness of annealing is measured with AFM is measured with annealing temperature variation relation for In-situ resistance rate Ge-Sb-C phase change film material thickness is stated in 200nm or so.The Ge-Sb-C phase-change thin films for x-ray albedo measurement Material thickness is in 20nm or so.Crystalline substance for x-ray albedo measurement and AFM the Ge-Sb-C phase change film materials measured Aspect product carry out annealing crystallization at 250 DEG C.The resistivity of the high-impedance state of the Ge-Sb-C phase-change storage materials is at least low-resistance 100 times of state resistivity.The Ge-Sb-C phase-change storage materials mix the content of C to control the phase change memory by control Phase transition temperature, the resistivity of material.The phase transition temperature of the Ge-Sb-C phase-change storage materials is improved significantly compared with Ge-Sb. The crystalline resistance rate of the Ge-Sb-C phase-change storage materials is improved compared with Ge-Sb.Mix the C's of different atomic percentage contents Ge-Sb-C phase-change storage materials before phase change after variable density can be down to 2% or so.When the atomic percentage content of doping C is higher than When 6%, first-principles calculations observed the formation of C chains, so C dopings also should not be too high.
The present invention provides a kind of preparation method of the Ge-Sb-C phase-change storage materials for phase transition storage, preparation sides Method includes magnetron sputtering method, chemical vapour deposition technique, atomic layer deposition method, galvanoplastic, electron-beam vapor deposition method etc..Wherein magnetic control splashes Shooting method preparation is the most flexible, and C, Ge, Sb target co-sputtering may be used, can also use C and GeiSbjCosputtering can also be adopted Ge after being adulterated with CiSbjAlloys target sputters, and can also use graphite flake being directly placed at GeiSbjAlloy target material is enterprising Row doping sputtering, these methods can prepare the Ge-Sb-C phase-change storage materials of the present invention according to the proportioning of chemical general formula.
Ge-Sb-C phase-change storage materials mature preparation process of the present invention, it is easy to accomplish with existing microelectronic process engineering Compatible, Ge-Sb-C phase-change storage materials of the invention not only inherit the advantages that Sb base phase-change storage material phase velocities are fast, together When also reduce before phase change after variable density, promote the cycling durable performance of device, Ge-Sb-C phase change memory materials of the invention Material also has higher phase transition temperature and higher crystalline resistance rate, is conducive to improve data retention, reduces power consumption.
It is embodiment below:
Embodiment 1
The chemical composition general formula of the nanometer Ge-Sb-C phase change film materials for phase transition storage prepared in the present embodiment For (GS)100-xCx, wherein GS represents Ge15Sb85, x=2.66 in the present embodiment.
Ge-Sb-C nano film materials are made using magnetron sputtering method;High-purity argon gas is passed through when preparation as sputter gas, Sputtering pressure is 0.5pa, Ge15Sb85Target uses DC power supply, power 30W, in Ge15Sb85It is placed at the etched rings of target The graphite flake of a piece of 1cm*1cm sizes is doped sputtering.Specific preparation method includes the following steps:
1. choosing the SiO that size is 1cm*1cm2/ Si (100) substrate, cleaning surface, the back side, removal dust granule, organic And inorganic impurity.
A) by SiO2/ Si (100) substrate is rinsed in acetone soln with the power ultrasonic 10 minutes of 40W, deionized water;
B) by treated substrate in ethanol solution with the power ultrasonic of 40w 10 minutes, deionized water is rinsed, high-purity N2Surface and the back side are done in air-blowing, obtain substrate to be sputtered.
2. being prepared (GS) using d.c. sputtering method97.34C2.66Prepare before film.
A) in Ge15Sb85The graphite flake of a piece of 1cm*1cm sizes is put at target material surface etched rings;
B) Ge for being placed with piece of graphite piece is installed15Sb85The purity of target, target reaches 99.99% (atomic percent), And base vacuum is evacuated to 10-4pa;
C) it uses high-purity Ar gas as sputter gas, sets Ar steady air currents and be adjusted to as 10sccm, and by sputtering pressure The distance 150mm of 0.5pa, target and substrate;
D) DC sputtering power power is set as 30W.
3. the method for magnetron sputtering is prepared (GS)97.34C2.66Nano phase change thin-film material.
A) space base support is rotated into Ge15Sb85Target position opens Ge15Sb85The baffle of target position carries out pre-sputtering 5-10min, clearly Clean target material surface;
b)Ge15Sb85After the completion of target material surface cleaning, Ge is closed15Sb85The baffle of target position rotates to substrate to be sputtered Ge15Sb85Target position opens Ge15Sb85Target position baffle, according to the sputtering time of setting, the Ge-Sb-C for starting to sputter different-thickness is thin Film.When sputtering time is 2min, (GS) that is prepared97.34C2.66Film thickness is 20nm or so, is used for X ray reflection rate It measures;When sputtering time is 15min, (GS) that is prepared97.34C2.66Film thickness is 200nm or so, for electricity in situ The annealing of resistance rate measures and AFM is measured.Film thickness is controlled by sputtering time, in Ge15Sb85When putting piece of graphite piece on target The sputter rate of film is 4.6s/nm.Through x-ray photoelectron spectroscopy (XPS) quantitative analysis, the change of the present embodiment thin-film material It is (GS) to learn composition formula97.34C2.66
Embodiment 2
The chemical composition general formula of the nano phase change thin-film material for phase transition storage prepared in the present embodiment is (GS)100-xCx, x=4.98 in the present embodiment.
Ge-Sb-C nano film materials are made using magnetron sputtering method;High-purity argon gas is passed through when preparation as sputter gas, Sputtering pressure is 0.5pa, Ge15Sb85Target uses DC power supply, power 30W, in Ge15Sb85It is placed at the etched rings of target The graphite flake of two panels 1cm*1cm sizes is doped sputtering.Specific preparation method includes the following steps:
1. choosing the SiO that size is 1cm*1cm2/ Si (100) substrate, cleaning surface, the back side, removal dust granule, organic And inorganic impurity.
A) by SiO2/ Si (100) substrate is rinsed in acetone soln with the power ultrasonic 10 minutes of 40W, deionized water;
B) by treated substrate in ethanol solution with the power ultrasonic of 40w 10 minutes, deionized water is rinsed, high-purity N2Surface and the back side are done in air-blowing, obtain substrate to be sputtered.
2. being prepared (GS) using d.c. sputtering method95.02C4.98Prepare before film.
A) in Ge15Sb85The graphite flake of two panels 1cm*1cm sizes is put at target material surface etched rings;
B) Ge for being placed with two panels graphite flake is installed15Sb85The purity of target, target reaches 99.99% (atomic percent), And base vacuum is evacuated to 10-4pa;
C) it uses high-purity Ar gas as sputter gas, sets Ar steady air currents and be adjusted to as 10sccm, and by sputtering pressure The distance 150mm of 0.5pa, target and substrate;
D) DC sputtering power power is set as 30W.
3. the method for magnetron sputtering is prepared (GS)95.02C4.98Nano phase change thin-film material.
A) space base support is rotated into Ge15Sb85Target position opens Ge15Sb85The baffle of target position carries out pre-sputtering 5-10min, clearly Clean target material surface;
b)Ge15Sb85After the completion of target material surface cleaning, Ge is closed15Sb85The baffle of target position rotates to substrate to be sputtered Ge15Sb85Target position opens Ge15Sb85Target position baffle, according to the sputtering time of setting, the Ge-Sb-C for starting to sputter different-thickness is thin Film.When sputtering time is 2min, (GS) that is prepared97.34C2.66Film thickness is 20nm or so, is used for X ray reflection rate It measures;When sputtering time is 20min, (GS) that is prepared95.02C4.98Film thickness is 200nm or so, for electricity in situ The annealing of resistance rate measures and AFM is measured.Film thickness is controlled by sputtering time, in Ge15Sb85When putting two panels graphite flake on target The sputter rate of film is 5.8s/nm.Through x-ray photoelectron spectroscopy (XPS) quantitative analysis, the change of the present embodiment thin-film material It is (GS) to learn composition formula95.02C4.98
Embodiment 3
The chemical composition general formula of the nano phase change thin-film material for phase transition storage prepared in the present embodiment is (GS)100-xCx, x=5.75 in the present embodiment.
Ge-Sb-C nano film materials are made using magnetron sputtering method;High-purity argon gas is passed through when preparation as sputter gas, Sputtering pressure is 0.5pa, Ge15Sb85Target uses DC power supply, power 30W, in Ge15Sb85It is placed at the etched rings of target The graphite flake of three pieces 1cm*1cm sizes is doped sputtering.Specific preparation method includes the following steps:
1. choosing the SiO that size is 1cm*1cm2/ Si (100) substrate, cleaning surface, the back side, removal dust granule, organic And inorganic impurity.
A) by SiO2/ Si (100) substrate is rinsed in acetone soln with the power ultrasonic 10 minutes of 40W, deionized water;
B) by treated substrate in ethanol solution with the power ultrasonic of 40w 10 minutes, deionized water is rinsed, high-purity N2Surface and the back side are done in air-blowing, obtain substrate to be sputtered.
2. being prepared (GS) using d.c. sputtering method94.25C5.75Prepare before film.
A) in Ge15Sb85The graphite flake of three pieces 1cm*1cm sizes is put at target material surface etched rings;
B) Ge for being placed with three pieces graphite flake is installed15Sb85The purity of target, target reaches 99.99% (atomic percent), And base vacuum is evacuated to 10-4pa;
C) it uses high-purity Ar gas as sputter gas, sets Ar steady air currents and be adjusted to as 10sccm, and by sputtering pressure The distance 150mm of 0.5pa, target and substrate;
D) DC sputtering power power is set as 30W.
3. the method for magnetron sputtering is prepared (GS)94.25C5.75Nano phase change thin-film material.
A) space base support is rotated into Ge15Sb85Target position opens Ge15Sb85The baffle of target position carries out pre-sputtering 5-10min, clearly Clean target material surface;
b)Ge15Sb85After the completion of target material surface cleaning, Ge is closed15Sb85The baffle of target position rotates to substrate to be sputtered Ge15Sb85Target position opens Ge15Sb85Target position baffle, according to the sputtering time of setting, the Ge-Sb-C for starting to sputter different-thickness is thin Film.When sputtering time is 3min, (GS) that is prepared94.25C5.75Film thickness is 20nm or so, is used for X ray reflection rate It measures;When sputtering time is 30min, (GS) that is prepared94.25C5.75Film thickness is 200nm or so, for electricity in situ The annealing of resistance rate measures and AFM is measured.Film thickness is controlled by sputtering time, in Ge15Sb85When putting three pieces graphite flake on target The sputter rate of film is 8.6s/nm.Through x-ray photoelectron spectroscopy (XPS) quantitative analysis, the change of the present embodiment thin-film material It is (GS) to learn composition formula94.25C5.75
Comparative example 1
Single layer Ge is prepared in this comparative example 115Sb85Phase change film material.
Ge15Sb85Nano film material is made using magnetron sputtering method;High-purity argon gas is passed through when preparation as sputter gas, Sputtering pressure is 0.5pa, Ge15Sb85Target uses DC power supply, power 30W.Specific preparation method includes the following steps:
1. SiO2/Si (100) substrate that size is 1cm*1cm is chosen, cleaning surface, the back side, removal dust granule, organic And inorganic impurity.
A) SiO2/Si (100) substrates and sheet glass are used to the power ultrasonic of 40w in acetone soln 10 minutes, deionization Water rinses;
B) by treated substrate in ethanol solution with the power ultrasonic of 40w 10 minutes, deionized water is rinsed, high-purity Surface and the back side are done in N2 air-blowings, obtain substrate to be sputtered.
2. preparing Ge using d.c. sputtering method15Sb85Prepare before film.
A) Ge is installed15Sb85The purity of target, target reaches 99.99% (atomic percent), and base vacuum is evacuated to 10-4Pa;
B) it uses high-purity Ar gas as sputter gas, sets Ar steady air currents and be adjusted to as 10sccm, and by sputtering pressure The distance 150mm of 0.5pa, target and substrate;
C) DC sputtering power power is set as 30W.
3. the method for magnetron sputtering prepares Ge15Sb85Nano phase change thin-film material.
A) space base support rotates to Ge15Sb85Target position opens Ge15Sb85The baffle of target carries out pre-sputtering 5-10min, cleans target Material surface;
b)Ge15Sb85After the completion of target surface cleaning, Ge is closed15Sb85The baffle of target rotates to substrate to be sputtered Ge15Sb85Target position opens Ge15Sb85Target position baffle starts to sputter Ge according to the sputtering time of setting15Sb85Film.Work as sputtering When time is 1min, the Ge that is prepared15Sb85Film thickness is 20nm or so, is measured for X ray reflection rate;When sputtering Between when being 10min, the Ge that is prepared15Sb85Film thickness is 200nm or so, for In-situ resistance rate annealing measurement and AFM It measures.Film thickness is controlled by sputtering time, and the sputter rate of film is 3s/nm.
Comparative example 2
As described in the background art, there are 10% vacancy in the crystalline state of conventional phase change material GST, thus before phase change after Density contrast can reach 8% or more.Liangcai Wu et al. are shown by X ray reflection rate measurement by GST phase transformation materials When adulterating C content to 2.9% in material, the variable density after before phase change can be reduced to 4.45% from 9.65%.In mechanism side Face, first-principles calculations of the Liangcai Wu et al. based on Density functional the result shows that, the C atoms of incorporation tend to replace For Te atoms, the spatial continuity of ABAB rings (A represents Ge or Sb atoms, and B represents Te atoms) is destroyed, increases tetrahedron Ge atoms Ratio reduce the variable density before and after material to improve the amorphous stability of GST.
And for the present invention Ge-Sb materials for, in crystalline state and be not present intrinsic vacancy, therefore before phase change after density Variation is originally just smaller than GST, 6% or so.And the present invention C doping contents concentration gradient from 2.66% to 5.75%, it can realize and variable density is down to 1.79% from 6.24%.And in terms of mechanism, in Ge-Sb phase-change materials not There are sulphur series elements Te, therefore C incorporations influence the GST different froms that the mechanism of Ge-Sb crystallization process should be adulterated with C, need to use Experiment and calculating research are explored.And further investigations have shown that, in Ge-Sb-C phase-change materials, C atoms are by being entrained in It in interstitial void, and forms tetrahedron center in amorphous state and improves atom packing efficiency, to the density after reduction before phase change Variation.
By (GS) of above-described embodiment 1, embodiment 2 and embodiment 397.34C2.66、(GS)95.02C4.98、(GS)94.25C5.75With The GS phase change film materials of comparative example 1 are tested, and obtain the front and back X ray reflection rate of each phase change film material annealing with incidence The diffraction curve at angle such as Fig. 1;By (GS) of above-described embodiment 1, embodiment 2 and embodiment 397.34C2.66、(GS)95.02C4.98、 (GS)94.25C5.75It is tested with the GS phase change film materials of comparative example 1, obtains using thickness before and after each phase change film material annealing The volume (density) of characterization changes the curve such as Fig. 2 changed with C doping contents.By above-described embodiment 1, embodiment 2 and embodiment 3 (GS)97.34C2.66、(GS)95.02C4.98、(GS)94.25C5.75It is tested, is obtained each with the GS phase change film materials of comparative example 1 The In-situ resistance rate of phase change film material and relation curve such as Fig. 3 of annealing temperature;With first-principles calculations when C doping contains Bond distance, bond angle and the ligancy situation such as Fig. 4 for the amorphous state Ge-Sb-C that amount is 5%;With first-principles calculations when C is adulterated The super born of the same parents' model such as Fig. 5 for the amorphous state Ge-Sb-C phase-change materials that content is 5%;Contained with the different C doping of first-principles calculations Formational situation such as Fig. 6 of C chains in the Ge-Sb-C phase-change storage materials of amount.The testing result of Fig. 1-Fig. 6 is as follows:
Fig. 1 is (GS) of the invention97.34C2.66、(GS)95.02C4.98、(GS)94.25C5.75With the GS phase-change thin films of comparative example 1 X ray reflection rate before and after anneal of material with incidence angle diffraction curve.Wherein, the deposition film that magnetron sputtering obtains is non- Crystalline state, after carrying out X ray reflection rate test, amorphous nano phase change film carries out annealing 10min at 250 DEG C.After annealing Crystalline state nano phase change film carry out the measurement of X ray reflection rate again, obtained by fitting and compare the close of the front and back film of annealing Degree and thickness change.The film measured for X ray reflection rate is single thin film of the thickness in 20nm or so, and film Surface roughness is 1nm or so, to meet test request.Can with it is seen in fig. 1, that when with one sheet of film annealing crystallization it Afterwards, critical angle and the corresponding angle of reflection of maximum intensity are deviated toward high angle, it is meant that the density of film increases, and thickness reduces (volume reduction).And according to the film thickness of X ray reflection rate and density measurement as a result, embodiment 1, embodiment 2 and embodiment 3 (GS)97.34C2.66、(GS)95.02C4.98、(GS)94.25C5.75It is preceding corresponding non-with the GS thin-film materials annealing for comparative example 1 Crystalline state density is respectively 6.15g/cm3、6.11g/cm3、6.07g/cm3And 6.19g/cm3, embodiment 1, embodiment 2 and embodiment 3 (GS)97.34C2.66、(GS)95.02C4.98、(GS)94.25C5.75It anneals at 250 DEG C with the GS thin-film materials for comparative example 1 Corresponding crystalline state density is respectively 6.49g/cm afterwards3、6.35g/cm3、6.27g/cm3And 6.58g/cm3, embodiment 1, embodiment 2 With (GS) of embodiment 397.34C2.66、(GS)95.02C4.98、(GS)94.25C5.75The front and back variable density difference of thin-film material annealing It is 5.53%, 3.89%, 3.29%, the variable density before and after the GS Thin-film anneals of comparative example 1 is 6.24%.It can be seen that after mixing C Ge-Sb-C films can effectively reduce the variable density before and after material phase transformation, reduce the stress generated in phase transition process, to It helps to ensure that PCRAM phase change mediums layer and upper/lower electrode reliable contacts, improves device cycle number and service life.
Fig. 2 is measured (GS) of the invention with AFM97.34C2.66、(GS)95.02C4.98、(GS)94.25C5.75With comparative example 1 The front and back volume (density) characterized with thickness of GS phase change film materials annealing changes the change curve with C content.For each C The film of doping concentration, it is (close come the volume for characterizing sample with thickness change after the front and back film thickness for respectively surveying 12 points of annealing Degree) variation, 12 variable densities are averaged (Δ ρtrans).Figure it is seen that embodiment 1, embodiment 2 and embodiment 3 (GS)97.34C2.66、(GS)95.02C4.98、(GS)94.25C5.75The front and back variable density of thin-film material annealing is respectively 4.89%, 3.80%, 1.79%, the variable density before and after the GS Thin-film anneals of comparative example 1 is 5.16%, the result and X-ray of variable density The result of reflectivity is consistent, it is seen that mixes C really and can effectively reduce the volume change in phase transition process, improve the cycle time of device Number and service life.
Fig. 3 is (GS) of the invention97.34C2.66、(GS)95.02C4.98、(GS)94.25C5.75With the GS phase-change thin films of comparative example 1 The In-situ resistance rate and annealing temperature relational graph of material, correspond to GeSb, (GS) respectively from left to right97.34C2.66、(GS)95.02C4.98 (GS)94.25C5.75.The In-situ resistance rate of each phase change film material and the relation test method of temperature are as follows:It is annealed by one The external M1500 tester of stove has built the test system of an in situ measurement resistance v. temperature.Annealing furnace passes through thermocouple pair Film sample is heated, and heating rate is 5 DEG C/min, while carrying out annealing operation under vacuum conditions.It is used while heating M1500 measures its resistance, and is converted into resistivity according to structural parameters.By Fig. 3, when less than phase transition temperature, all films are equal For high-impedance state, show that all thin-film materials are amorphous state.As temperature gradually rises, film resiativity gradually slowly reduces, When it reaches phase transition temperature, film resiativity drastically declines, and is held essentially constant after reaching a certain resistivity value, shows thin The phase structure of membrane material is converted into the trigonal crystal structure of the typical Sb atoms of crystalline state from amorphous state.As shown in Figure 3:First, with The increase of C content is mixed, the phase transition temperature of thin-film material has been increased to 210 DEG C from 175 DEG C in comparative example 1, has shown phase-change material The thermal stability of Ge-Sb-C is significantly improved;Second, with the increase for mixing C content, the crystalline resistance rate of phase change film material Increase, effectively reduces RESET power consumptions;Third, with the increase for mixing C content, phase change film material Ge-Sb-C amorphous state high resistants Order of magnitude comparison is kept between crystalline state low-resistance, is conducive to the signal-to-noise ratio for improving PCRAM, is improved its anti-interference ability.
Fig. 4 is with the bond distance of the amorphous state Ge-Sb-C for being 5% when C doping contents of first-principles calculations, bond angle and to match Digit situation.It can be found that the bond distance of C and Sb is obviously (Fig. 4 a) shorter than the bond distance of Ge-Ge, Ge-Sb and Sb-Sb;And C is former Son is formed by bond angle close to 109 ° (Fig. 4 b);It is found according to ligancy result of calculation, the ligancy of C atoms is 4 (Fig. 4 c), card It is bright in Ge-Sb-C, the C atoms of incorporation form tetrahedron center, more stable chemical bond are formed with Ge/Sb, as used in Fig. 5 Shown in super born of the same parents' model of the amorphous state Ge-Sb-C phase-change materials for being 5% when C doping contents of first-principles calculations.It can be seen that C Doping improves the deposition efficiency of amorphous atomic, to the variable density after reducing before phase change.
Fig. 6 is in the present invention with C in the Ge-Sb-C phase-change storage materials of the different C doping contents of first-principles calculations The formational situation of chain.It can be found that when C doping contents are 3% (Fig. 6 b), C atoms are randomly dispersed in the week of Ge and Sb atoms It encloses, and C atoms do not form chemical bond between each other;When C doping contents are 6% (Fig. 6 c), a small amount of C can be obviously observed The formation of chain, but most of C atoms still with Ge/Sb bondings;And work as C doping contents in 10% or so (Fig. 6 d), it can be found that greatly Part C atoms are in key and form apparent C chains.The formation of C chains can lead to the precipitation of C in phase transition process, influence following for device Ring performance, and this with the purpose of the present invention is disagree.Therefore, the atom doped contents of currently preferred C are 2%- 6% or so doping concentration, to achieve the purpose that variable density after reducing before phase change and keep Ge-Sb other materials performances.
As it will be easily appreciated by one skilled in the art that the foregoing is merely illustrative of the preferred embodiments of the present invention, not to The limitation present invention, all within the spirits and principles of the present invention made by all any modification, equivalent and improvement etc., should all include Within protection scope of the present invention.

Claims (10)

1. a kind of Ge-Sb-C phase-change storage materials, which is characterized in that its chemical composition general formula is (GeiSbj)100-xCx, wherein x, I, j are atomic percent, wherein 0 < x <, 15,0 < i≤50,50≤j < 100, i+j=100.
2. phase-change storage material as described in claim 1, which is characterized in that 0 < x <, 6,0 < i≤20,80≤j < 100, i+ J=100.
3. phase-change storage material as claimed in claim 1 or 2, which is characterized in that C in the Ge-Sb-C phase-change storage materials Atom is present in Ge-Sb interstitial voids, and forms chemical bond with Ge-Sb.
4. phase-change storage material as claimed in claim 1 or 2, which is characterized in that the Ge-Sb-C phase-change storage materials are Ge-Sb-C phase change film materials.
5. phase-change storage material as claimed in claim 4, which is characterized in that the thickness of the film is 20-200nm.
6. phase-change storage material as claimed in claim 1 or 2, which is characterized in that the Ge-Sb-C phase-change storage materials pass through The incorporation content of C is controlled to control the phase transition temperature and resistivity of the phase-change storage material.
7. phase-change storage material as claimed in claim 1 or 2, which is characterized in that the height of the Ge-Sb-C phase-change storage materials The resistivity of resistance state is at least 100 times of low resistance state.
8. the preparation method of the phase-change storage material as described in claim 1-7 any one, which is characterized in that it is splashed for magnetic control Penetrate method, chemical vapour deposition technique, atomic layer deposition method, galvanoplastic or electron-beam vapor deposition method.
9. preparation method as claimed in claim 8, which is characterized in that it is magnetron sputtering method, and specific magnetron sputtering mode is Any one in following four mode:(1) C, Ge and Sb target co-sputtering;(2) C and GeiSbjCosputtering;(3) after C doping GeiSbjAlloys target sputters and graphite flake is directly placed at Ge by (4)iSbjSputtering is doped on alloy target material.
10. application of the Ge-Sb-C phase-change storage materials in phase transition storage as described in claim 1-7 is any.
CN201810097825.8A 2018-01-31 2018-01-31 A kind of Ge-Sb-C phase-change storage material, preparation method and application Active CN108346739B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201810097825.8A CN108346739B (en) 2018-01-31 2018-01-31 A kind of Ge-Sb-C phase-change storage material, preparation method and application

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201810097825.8A CN108346739B (en) 2018-01-31 2018-01-31 A kind of Ge-Sb-C phase-change storage material, preparation method and application

Publications (2)

Publication Number Publication Date
CN108346739A true CN108346739A (en) 2018-07-31
CN108346739B CN108346739B (en) 2019-09-13

Family

ID=62961473

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201810097825.8A Active CN108346739B (en) 2018-01-31 2018-01-31 A kind of Ge-Sb-C phase-change storage material, preparation method and application

Country Status (1)

Country Link
CN (1) CN108346739B (en)

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109860388A (en) * 2019-01-09 2019-06-07 江苏理工学院 Multi-layer phase change film and preparation method and application
CN110556475A (en) * 2019-08-16 2019-12-10 华中科技大学 Low-density variable phase-change material, phase-change memory and preparation method
CN110571327A (en) * 2019-08-09 2019-12-13 华中科技大学 Cr-Sb phase change storage material and preparation and application thereof
CN110718628A (en) * 2019-09-03 2020-01-21 华中科技大学 Phase change alloy material, phase change memory and preparation method of phase change alloy material
CN110911557A (en) * 2019-10-30 2020-03-24 华中科技大学 Doped Ge-Sb phase change material, phase change memory and preparation method thereof
WO2021083010A1 (en) * 2019-10-28 2021-05-06 华中科技大学 Superlattice phase-change thin film with low density change, phase-change memory and preparation method therefor
CN113072915A (en) * 2021-03-24 2021-07-06 华中科技大学 Sb based on oxygen doping2Te3Phase change material, phase change memory and preparation method

Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2004363541A (en) * 2003-05-09 2004-12-24 Mitsubishi Materials Corp Phase change recording film high in electric resistance, and sputtering target for forming the film
JP2006245251A (en) * 2005-03-03 2006-09-14 Mitsubishi Materials Corp Phase change recording film with stable amorphous state, and sputtering target for forming it
US20090250682A1 (en) * 2008-04-08 2009-10-08 Samsung Electronics Co., Ltd. Phase change memory device
CN101582485A (en) * 2009-06-15 2009-11-18 中国科学院上海微系统与信息技术研究所 Doping modified phase change material and phase change storage unit containing same and preparation method thereof
CN101931049A (en) * 2010-08-31 2010-12-29 中国科学院上海微系统与信息技术研究所 Anti-fatigue phase change storage unit with low power consumption and preparation method thereof
CN103855300A (en) * 2012-12-04 2014-06-11 中芯国际集成电路制造(上海)有限公司 Phase change storage and forming method thereof
CN106257700A (en) * 2015-06-19 2016-12-28 旺宏电子股份有限公司 Ovonics unified memory material, phase-change memorizer device and manufacture method thereof
CN106299113A (en) * 2016-08-22 2017-01-04 中国科学院上海微系统与信息技术研究所 Ge Sb Se phase-change material, phase-changing memory unit and preparation method thereof
CN106992196A (en) * 2016-01-13 2017-07-28 三星电子株式会社 Variable resistance memory device

Patent Citations (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2004363541A (en) * 2003-05-09 2004-12-24 Mitsubishi Materials Corp Phase change recording film high in electric resistance, and sputtering target for forming the film
JP2006245251A (en) * 2005-03-03 2006-09-14 Mitsubishi Materials Corp Phase change recording film with stable amorphous state, and sputtering target for forming it
US20090250682A1 (en) * 2008-04-08 2009-10-08 Samsung Electronics Co., Ltd. Phase change memory device
CN101582485A (en) * 2009-06-15 2009-11-18 中国科学院上海微系统与信息技术研究所 Doping modified phase change material and phase change storage unit containing same and preparation method thereof
CN101931049A (en) * 2010-08-31 2010-12-29 中国科学院上海微系统与信息技术研究所 Anti-fatigue phase change storage unit with low power consumption and preparation method thereof
CN103855300A (en) * 2012-12-04 2014-06-11 中芯国际集成电路制造(上海)有限公司 Phase change storage and forming method thereof
CN106257700A (en) * 2015-06-19 2016-12-28 旺宏电子股份有限公司 Ovonics unified memory material, phase-change memorizer device and manufacture method thereof
CN106992196A (en) * 2016-01-13 2017-07-28 三星电子株式会社 Variable resistance memory device
CN106299113A (en) * 2016-08-22 2017-01-04 中国科学院上海微系统与信息技术研究所 Ge Sb Se phase-change material, phase-changing memory unit and preparation method thereof

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
ANDRZEJ KUSIAK等: "Thermal conductivity of carbon doped GeTe thin films in amorphous and crystalline state measured by modulated photo thermal radiometry", 《JOURNAL OF PHYSICS: CONFERENCE SERIES 》 *
WANGYANG ZHOU等: "High thermal stability and low density variation of carbon-doped Ge2Sb2Te5 for phase-change memory application", 《APPLIED PHYSICS LETTERS》 *

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN109860388A (en) * 2019-01-09 2019-06-07 江苏理工学院 Multi-layer phase change film and preparation method and application
CN110571327A (en) * 2019-08-09 2019-12-13 华中科技大学 Cr-Sb phase change storage material and preparation and application thereof
CN110556475A (en) * 2019-08-16 2019-12-10 华中科技大学 Low-density variable phase-change material, phase-change memory and preparation method
CN110556475B (en) * 2019-08-16 2021-06-08 华中科技大学 Low-density variable phase-change material, phase-change memory and preparation method
CN110718628A (en) * 2019-09-03 2020-01-21 华中科技大学 Phase change alloy material, phase change memory and preparation method of phase change alloy material
CN110718628B (en) * 2019-09-03 2022-03-08 华中科技大学 Phase change alloy material, phase change memory and preparation method of phase change alloy material
WO2021083010A1 (en) * 2019-10-28 2021-05-06 华中科技大学 Superlattice phase-change thin film with low density change, phase-change memory and preparation method therefor
CN110911557A (en) * 2019-10-30 2020-03-24 华中科技大学 Doped Ge-Sb phase change material, phase change memory and preparation method thereof
WO2021082808A1 (en) * 2019-10-30 2021-05-06 华中科技大学 Doped ge-sb-based phase change material, phase change memory and preparation method therefor
CN113072915A (en) * 2021-03-24 2021-07-06 华中科技大学 Sb based on oxygen doping2Te3Phase change material, phase change memory and preparation method
CN113072915B (en) * 2021-03-24 2022-03-11 华中科技大学 Sb based on oxygen doping2Te3Phase change material, phase change memory and preparation method

Also Published As

Publication number Publication date
CN108346739B (en) 2019-09-13

Similar Documents

Publication Publication Date Title
CN108346739B (en) A kind of Ge-Sb-C phase-change storage material, preparation method and application
Chung et al. Investigation of SnSe, SnSe2, and Sn2Se3 alloys for phase change memory applications
Kang et al. Structural transformation of SbxSe100− x thin films for phase change nonvolatile memory applications
CN106410025A (en) Oxygen-doped Sb nanometer phase change thin-film materials and preparation method thereof and application thereof
CN112687359B (en) Screening and matching method for insulating heat-insulating material and nanocrystalline metal material in nano current channel layer
CN101299454A (en) Method for preparing nano composite phase-changing material
Zhang et al. Characteristics of Si-doped Sb2Te3 thin films for phase-change random access memory
WO2024001426A1 (en) Phase-change thin film, thin film preparation method, and phase-change memory
CN113072915B (en) Sb based on oxygen doping2Te3Phase change material, phase change memory and preparation method
Wang et al. Ge/Sb2Te3 nanocomposite multilayer films for high data retention phase-change random access memory application
Kim et al. Effects of N2+ ion implantation on phase transition in Ge2Sb2Te5 films
Wu et al. Development of Sb2Se3 alloys by Ti-doping with ultralow resistance drift and improved microstructure for nonvolatile memory applications
CN102610745B (en) Si-Sb-Te based sulfur group compound phase-change material for phase change memory
CN111876731B (en) Ca-doped antimony telluride ultrastable phase change storage thin film material and preparation method thereof
Ren et al. Study on the crystallization behaviors of Si2Sb2Tex materials
Kumar et al. Optical properties and phase transition in photodoped amorphous Ge–Sb–Te: Ag thin films
Ume et al. Electrical and structural properties of binary Ga–Sb phase change memory alloys
CN106374042A (en) Nitrogen-doped Sb nano phase change thin film material and preparation method and application thereof
Ta et al. Phase transition behavior and electronic properties of GaSb/Ge2Sb2Te5 superlattice-like structure thin films
Feng et al. Multi-step phase-change behavior in Ga30Sb70/SnSe2 nanocomposite multilayer thin films
CN107546325B (en) Composite film phase-change material
CN110571327B (en) Cr-Sb phase change storage material and preparation and application thereof
CN112786782B (en) Sb-Si for phase change memory 3 N 4 Thin film material and preparation method thereof
CN110729401B (en) Ga-Sb-O phase-change material and application and preparation method thereof
Kim et al. Characterization of Agx (Ge2Sb2Te5) 1− xthin film by RF magnetron sputtering

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant